A semiconductor device includes a substrate, a channel layer formed over the substrate, an active layer formed over the channel layer, and a gate structure formed over the active layer. The active layer is configured to cause a two dimensional electron gas (2DEG) to be formed in the channel layer along an interface between the channel layer and the active layer. The gate structure is configured to deplete the 2DEG under the gate structure. The active layer has a negatively charged region under the gate structure. The negatively charged region is configured to further deplete the 2DEG under the gate structure.
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1. A semiconductor device, comprising:
a substrate;
a channel layer formed over the substrate;
an active layer formed over the channel layer, the active layer configured to cause a two dimensional electron gas (2DEG) to be formed in the channel layer along an interface between the channel layer and the active layer; and
a gate structure formed over the active layer, the gate structure configured to deplete the 2DEG under the gate structure;
wherein the active layer has a negatively charged region under the gate structure, the negatively charged region configured to further deplete the 2DEG under the gate structure.
13. A method of manufacturing a semiconductor device, the method comprising:
forming a channel layer over a substrate;
forming an active layer over the channel layer, the active layer configured to cause a two dimensional electron gas (2DEG) to be formed in the channel layer along an interface between the channel layer and the active layer;
forming a negatively charged region in a gate area of the active layer, the negatively charged region configured to deplete the 2DEG under the gate area; and
forming a gate structure over the gate area of the active layer, the gate structure configured to further deplete the 2DEG under the gate area.
6. A high electron mobility transistor (HEMT), comprising:
a semiconductor substrate;
a buffer layer formed over the semiconductor substrate;
a channel layer formed over the buffer layer, the channel layer comprising GaN;
an active layer formed over the channel layer, the active layer comprising AlGaN;
a gate structure formed over the active layer, the gate structure comprising:
a p-doped layer formed over the active layer,
an n-doped layer formed over the p-doped layer, and
a gate electrode formed over the n-doped layer; and
a source electrode and a drain electrode formed over the channel layer;
wherein the active layer has a negatively charged region under the gate structure, the negatively charged region including negative ions.
2. The semiconductor device of
3. The semiconductor device of
4. The semiconductor device of
5. The semiconductor device of
7. The HEMT of
8. The HEMT of
9. The HEMT of
10. The HEMT of
11. The HEMT of
the buffer layer comprises:
a first AlN layer formed over the semiconductor substrate; and
a plurality of first AlGaN layers formed over the first AlN layer and under the channel layer, the plurality of first AlGaN layers having an Al concentration reducing toward the channel layer, and
the active layer comprises:
a second AlN layer formed over the channel layer; and
a second AlGaN layer formed over the second AlN layer.
12. The HEMT of
a passivation layer formed over the active layer, the passivation layer surrounding the gate structure.
14. The method of
15. The method of
16. The method of
17. The method of
forming a passivation layer over the active layer; and
implanting negative ions, through the passivation layer, into the gate area of the active layer underlying the passivation layer to form the negatively charged region in the gate area.
18. The method of
removing an area of the passivation layer over the gate area to expose the negatively charged region;
forming a p-doped layer over the exposed negatively charged region; and
forming an n-doped layer over the p-doped layer, wherein the p-doped layer and the n-doped layer define the gate structure.
19. The method of
forming a p-doped layer over the active layer,
forming an n-doped layer over the p-doped layer,
implanting negative ions, through the n-doped layer and the p-doped layer, into the gate area of the active layer underlying the p-doped layer and n-doped layer to form the negatively charged region in the gate area.
20. The method of
removing the p-doped layer and n-doped layer outside the gate area, wherein the p-doped layer and the n-doped layer remaining over the gate area define the gate structure; and
forming a passivation layer around the gate structure.
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The instant application is related to the following U.S. patent applications:
U.S. Patent Application titled “TRANSISTOR HAVING PARTIALLY OR WHOLLY REPLACED SUBSTRATE AND METHOD OF MAKING THE SAME,” Ser. No. 13/944,779;
U.S. Patent Application titled “TRANSISTOR HAVING HIGH BREAKDOWN VOLTAGE AND METHOD OF MAKING THE SAME,” Ser. No. 13/944,713;
U.S. Patent Application titled “TRANSISTOR HAVING BACK-BARRIER LAYER AND METHOD OF MAKING THE SAME,” Ser. No. 13/944,584;
U.S. Patent Application titled “TRANSISTOR HAVING DOPED SUBSTRATE AND METHOD OF MAKING THE SAME,” Ser. No. 13/944,494;
U.S. Patent Application titled “TRANSISTOR HAVING A BACK-BARRIER LAYER AND METHOD OF MAKING THE SAME,” Ser. No. 944,672; and
U.S. Patent Application titled “TRANSISTOR HAVING OHMIC CONTACT BY GRADIENT LAYER AND METHOD OF MAKING SAME” Ser. No. 14/010,268; and
U.S. Patent Application titled “TRANSISTOR HAVING AN OHMIC CONTACT BY SCREEN LAYER AND METHOD OF MAKING THE SAME” Ser. No. 14/010,220.
U.S. Patent Application titled “TRANSISTOR HAVING METAL DIFFUSION BARRIER AND METHOD OF MAKING THE SAME” Ser. No. 13/948,925.
The entire contents of the above-referenced applications are incorporated by reference herein.
Due to high current density, high breakdown voltage, and low ON resistance, High Electron Mobility Transistors (HEMTs) are suitable for use in power applications. A HEMT structure includes a channel layer and an active layer. A two-dimensional electron gas (2DEG) is generated in the channel layer, adjacent an interface with the active layer. The 2DEG is used in the HEMT structure as charge carriers. The 2DEG is generated even in the absence of a voltage applied to the HEMT structure. Thus, a HEMT structure is, by nature, a normally ON structure with a negative threshold voltage. A consideration in designing circuitry for power applications involves converting a normally ON HEMT structure to a normally OFF HEMT structure with a positive threshold voltage.
One or more embodiments are illustrated by way of example, and not by limitation, in the figures of the accompanying drawings, wherein elements having the same reference numeral designations represent like elements throughout. The drawings are not to scale, unless otherwise disclosed.
It is to be understood that the following disclosure provides many different embodiments or examples, for implementing different features of various embodiments. Specific examples of components and arrangements are described below to simplify the present disclosure. An inventive concept may; however, be embodied in many different forms and should not be construed as being limited to the embodiments set forth herein. It will be apparent; however, that one or more embodiments may be practiced without these specific details. Like reference numerals in the drawings denote like elements.
In some embodiments, in order to convert a normally ON HEMT structure to a normally OFF HEMT structure, a gate structure formed over the active layer is configured to deplete the 2DEG under the gate structure. To further deplete the 2DEG, a negatively charged region is formed in the active layer, under the gate structure. As a result, the HEMT structure in accordance with some embodiments achieves an increase in the threshold voltage, without decreasing the carrier density in the 2DEG and/or increasing the channel resistance (RS). The described technique is suitable not only for HEMT structures, but also for other types of semiconductor devices which use 2DEGs as charge carriers.
In some embodiments, the substrate 110 includes a silicon carbide (SiC) substrate, sapphire substrate, or a silicon substrate. In at least one embodiment, the substrate 110 includes a Si(111) wafer to provide an optimal lattice mismatch with an overlying layer, such as a GaN layer described herein.
In some embodiments, the buffer layer 120 includes a nucleation layer over the substrate 110. The nucleation layer has a lattice structure and/or a thermal expansion coefficient (TEC) suitable for bridging the lattice mismatch and/or the TEC mismatch between the substrate 110 and an overlying layer, such as the channel layer 130. In some embodiments, the nucleation layer includes aluminum nitride (AlN). In some embodiments, the nucleation layer has a thickness of 70 to 300 nanometers (nm). In some embodiments, the nucleation layer is omitted.
In some embodiments, the buffer layer 120 includes a transition layer over the nucleation layer, or over the substrate 110 in one or more embodiments where the nucleation layer is omitted. The transition layer further facilitates gradual changes of lattice structures and TECs between the nucleation layer (or the substrate 110) and the channel layer 130. In some embodiments, the transition layer includes a graded aluminum-gallium nitride (AlxGa(1-x)N, x is the aluminum content ratio in the aluminum-gallium constituent) layer. In some embodiments, the graded aluminum gallium nitride layer includes multiple layers each having a decreased ratio x (from a bottom layer adjoining the nucleation layer to a top layer adjoining the channel layer 130. In at least one embodiment, the graded aluminum gallium nitride layer has three layers having the x ratio in the range of 0.7-0.9 for the bottom layer, in the range of 0.4-0.6 for a middle layer, and in the range of 0.15-0.3 for the top layer. In some embodiments, instead of having multiple layers with different x ratios, the graded aluminum gallium nitride layer has a continuous gradient of the ratio x. In some embodiments, the transition layer has a thickness of 500 to 1050 nm. In some embodiments, the transition layer is omitted.
In some embodiments, the channel layer 130 includes one or more III-V compound layers. One or more of the III-V compound layers is doped in at least one embodiment. In one or more embodiments, the channel layer 130 includes alternatingly arranged p-doped and n-doped III-V compound layers. In at least one embodiment, the channel layer 130 includes a C-doped GaN layer. In some embodiments, the channel layer 130 has a thickness of 500 to 5000 nm.
The active layer 140 includes one or more III-V compound layers which are different from the III-V compound layers of the channel layer 130 in composition. In some embodiments, the active layer 140 comprises AlN, AlyGa(1-y)N (where y is the aluminum content ratio), or a combination thereof. The active layer 140 is configured to cause a 2DEG to be formed in the channel layer 130 along an interface 141 between the channel layer 130 and the active layer 140. A heterojunction is formed between the active layer 140 and the channel layer 130 having two different semiconductor materials. A band gap discontinuity exists between the active layer 140 and the channel layer 130. The electrons from a piezoelectric effect in the active layer 140 drop into the channel layer 130, and thus create a thin layer 143 of highly mobile conducting electrons, i.e., the 2DEG, in the channel layer 130, adjacent the interface 141 with the active layer 140. The electrons in the 2DEG are charge carriers in the channel layer 130. When a voltage is applied to the gate electrode 186, it is possible to modulate a current (i.e., a drain current) flowing through the channel layer 130, from the drain electrode 184 to the source electrode 182.
The 2DEG is generated naturally at the interface 141 of different III-V compound materials forming the heterojunction between the channel layer 130 and the active layer 140. Due to the naturally occurring 2DEG and without the negatively charged region 160 and/or the gate structure 170, the semiconductor device 100 would be conductive without the application of a voltage to the gate electrode 186, i.e., the semiconductor device 100 would be a normally ON device. A gate-source voltage versus drain current relationship 191 of a normally ON HEMT structure, which has a negative threshold voltage VT1, is shown in
In some embodiments, to convert a normally ON HEMT structure to a normally OFF HEMT structure, a gate structure formed over the active layer is configured to deplete the 2DEG under the gate structure. For example, the gate structure 170 formed over the active layer 140 is configured to deplete the 2DEG under the gate structure 170, i.e., the 2DEG is depleted in an area 144 under the gate structure 170, leaving the 2DEG in areas 145, 146, between (i) the gate structure 170 and (ii) the source electrode 182 and the drain electrode 184, respectively. The gate structure 170 includes the p-doped layer 172 over the active layer 140, and the n-doped layer 174 over the p-doped layer 172. Example materials for the p-doped layer 172 and/or the n-doped layer 174 include, but are not limited to, GaN, AlGaN, InGaN and InAlGaN. Examples of p-type dopants include, but are not limited to, carbon, iron, magnesium, and zinc. Examples of n-type dopants include, but are not limited to, silicon and oxygen. In at least one embodiment, the n-doped layer 174 is omitted.
The p-doped layer 172, e.g., p-doped GaN or p-GaN, and the active layer 140, e.g., AlyGa(1-y)N, together form a PN junction over the area 144. Such a PN junction depletes the 2DEG in the area 144 under the gate structure 170, when no voltage is applied to the semiconductor device 100. In at least one embodiment where the n-doped layer 174 is provided, the n-doped layer 174, e.g., n-doped GaN or n-GaN, defines together with the p-doped layer 172 and the active layer 140, an NPN junction which also depletes the 2DEG in the area 144 under the gate structure 170. The n-doped layer 174 is further configured as a contact layer between the p-doped layer 172 and the gate electrode 186. Because the PN or NPN junction depletes the 2DEG in the area 144 under the gate structure 170, the 2DEG is interrupted in the area 144 and current is no longer flowing in the semiconductor device 100 when no voltage is applied to the semiconductor device 100. The semiconductor device 100 with the gate structure 170 is a normally OFF HEMT structure, which has a gate-source voltage versus drain current relationship 193 with a positive threshold voltage VT2, as shown in
Although the semiconductor device 100 with the gate structure 170 is a normally OFF HEMT structure suitable for power applications, in some situations, the positive threshold voltage VT2 provided by the gate structure 170 is insufficient. In some embodiments, to further increase the threshold voltage of the semiconductor device 100, the negatively charged region 160 is provided in the active layer 140, under the gate structure 170. In at least one embodiment, the negatively charged region 160 includes negative ions implanted into a gate area of the active layer 140 under the gate structure 170, i.e., over the area 144. Examples of negative ions in the negatively charged region 160 include, but are not limited to, ions of one or more of F, Mg, Fe, C and Zn. The negative ions electrostatically repel electrons in the 2DEG further away from the area 144 under the negatively charged region 160. In other words, the negatively charged region 160 further deplete the 2DEG under the gate structure 170. The semiconductor device 100 with both the gate structure 170 and the negatively charged region 160 has a gate-source voltage versus drain current relationship 195 shown in
Compared to other approaches, the higher threshold voltage VT3 is achieved in the semiconductor device 100 in accordance with some embodiments, without decreasing the carrier density in the 2DEG and/or increasing the channel resistance. For example, to increase the threshold voltage of a HEMT structure, the other approaches propose reducing the thickness and/or the aluminum content ratio of AlGaN in the active layer. However, a reduction in thickness or aluminum content ratio of AlGaN in the active layer also reduces the electron density of the 2DEG which, in turn, results in an increased channel resistance and/or a lower current flowing through the HEMT structure. Such an increased channel resistance and/or reduced current are design concerns in various power applications. By increasing the threshold voltage without decreasing the carrier density in the 2DEG and/or increasing the channel resistance, the semiconductor device 100 in accordance with some embodiments is advantageous over HEMT structures of the other approaches described herein.
At operation 205 in
As shown in
The buffer layer 320 includes a transition layer 324 formed over the nucleation layer 322, or over the substrate 310 in at least one embodiment where the nucleation layer 322 is not formed. In some embodiments, the transition layer 324 is a graded aluminum-gallium nitride AlxGa(1-x)N layer. In some embodiments, the graded aluminum gallium nitride layer has two or more of aluminum-gallium nitride layers each having a different ratio x decreased from the bottom to the top. In some embodiments, each of the two or more of aluminum-gallium nitride layers is formed by a MOCVD process, using aluminum-containing precursor, gallium-containing precursor, and nitrogen-containing precursor. In some embodiments, the aluminum-containing precursor includes TMA, TEA, or other suitable chemical. In some embodiments, the gallium-containing precursor includes trimethylgallium (TMG), triethylgallium (TEG), or other suitable chemical. In some embodiments, the nitrogen-containing precursor includes ammonia, TBAm, phenyl hydrazine, or other suitable chemical. In at least one embodiment, the transition layer 324 includes a bottom AlGaN layer 327, a middle AlGaN layer 328 and a top AlGaN layer 329. The bottom AlGaN layer 327 has the aluminum content ratio x of 0.7 to 0.9 and is formed, e.g., grown, at a temperature of 1000 to 1200° C. to a thickness of 50 to 200 nm. The middle AlGaN layer 328 has the aluminum content ratio x of 0.4 to 0.6 and is formed, e.g., grown, at a temperature of 1000 to 1200° C. to a thickness of 150 to 250 nm. The top AlGaN layer 329 has the aluminum content ratio x of 0.15 to 0.3 and is formed, e.g., grown, at a temperature of 1000 to 1200° C. to a thickness of 350 to 650 nm. Other numbers of AlGaN layers and/or aluminum content ratios in individual AlGaN layers are within the scope of various embodiments. In some embodiments, the graded aluminum gallium nitride layer has a continuous gradient of the ratio x gradually decreased from the bottom to the top and is formed by a MOCVD process. In some embodiments, the transition layer 324 and the operation for forming the transition layer 324 are omitted.
The channel layer 330 includes one or more III-V compound layers formed over substrate 310, the nucleation layer 322, and/or the transition layer 324. One or more of the III-V compound layers is doped in at least one embodiment. For example, the channel layer 330 in at least one embodiment includes C-doped GaN. In some embodiments, the channel layer 330 is formed, e.g., grown, by a MOCVD process using gallium-containing precursor and nitrogen-containing precursor, at a temperature of 1000 to 1200° C. to a thickness of 500-5000 nm.
The active layer 340 is formed over the channel layer 330. In some embodiments, the active layer 340 includes AlGaN, aluminum-gallium Arsenide (AlGaAs), aluminum-Indium phosphide (AlInP), or a combination thereof. In some embodiments, the active layer 340 is formed by a MOCVD process, using aluminum-containing precursor, gallium-containing precursor, and nitrogen-containing precursor. In at least one embodiment, the active layer 340 includes a lower AlN layer 341 and an upper AlyGa(1-y)N layer 342. The lower AlN layer 341 is formed, e.g., grown, at a temperature of 1000 to 1200° C. to a thickness of 0.5 to 1.5 nm. The upper AlyGa(1-y)N layer 342 has the aluminum content ratio of 0.1 to 0.3 and is formed, e.g., grown, at a temperature of 1000 to 1200° C. to a thickness of 10 to 40 nm.
The passivation layer 350 is formed over the active layer 340. Examples of materials for the passivation layer 350 include, but are not limited to, silicon nitride, silicon oxide, and silicon oxynitride. In at least one embodiment, the passivation layer 350 is SiN formed by chemical vapor deposition (CVD) to a thickness of 100 nm.
At operation 215 in
As shown in
At operation 225 in
As shown in
At operation 235 in
As shown in
At operation 245 in
As shown in
In the method described with respect to
At operation 405 in
At operation 415 in
As shown in
At operation 425 in
As shown in
At operation 435 in
The above methods include example operations, but they are not necessarily required to be performed in the order shown. Operations may be added, replaced, changed order, and/or eliminated as appropriate, in accordance with the spirit and scope of embodiments of the disclosure. Embodiments that combine different features and/or different embodiments are within the scope of the disclosure and will be apparent to those of ordinary skill in the art after reviewing this disclosure.
According to some embodiments, a semiconductor device comprises a substrate, a channel layer formed over the substrate, an active layer formed over the channel layer, and a gate structure formed over the active layer. The active layer is configured to cause a two dimensional electron gas (2DEG) to be formed in the channel layer along an interface between the channel layer and the active layer. The gate structure is configured to deplete the 2DEG under the gate structure. The active layer has a negatively charged region under the gate structure. The negatively charged region is configured to further deplete the 2DEG under the gate structure.
According to some embodiments, a High Electron Mobility Transistor (HEMT) comprises a semiconductor substrate, a buffer layer formed over the semiconductor substrate, a channel layer formed over the buffer layer, an active layer formed over the channel layer, a gate structure formed over the active layer, and a source electrode and a drain electrode formed over the channel layer. The channel layer comprises GaN. The active layer comprises AlGaN. The gate structure comprises a p-doped layer formed over the active layer, an n-doped layer formed over the p-doped layer, and a gate electrode formed over the n-doped layer. The active layer has a negatively charged region under the gate structure. The negatively charged region includes negative ions.
In a method of manufacturing a semiconductor device in accordance with some embodiments, a channel layer is formed over a substrate. An active layer is formed over the channel layer. The active layer is configured to cause a two dimensional electron gas (2DEG) to be formed in the channel layer along an interface between the channel layer and the active layer. A negatively charged region is formed in a gate area of the active layer. The negatively charged region is configured to deplete the 2DEG under the gate area. A gate structure is formed over the gate area of the active layer. The gate structure is configured to further deplete the 2DEG under the gate area.
It will be readily seen by one of ordinary skill in the art that one or more of the disclosed embodiments fulfill one or more of the advantages set forth above. After reading the foregoing specification, one of ordinary skill will be able to affect various changes, substitutions of equivalents and various other embodiments as broadly disclosed herein. It is therefore intended that the protection granted hereon be limited only by the definition contained in the appended claims and equivalents thereof.
Liu, Po-Chun, Chen, Chi-Ming, Yu, Chung-Yi
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